{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:M4W3Y2VA2KGQA4BVGFTVZC2ETN","short_pith_number":"pith:M4W3Y2VA","schema_version":"1.0","canonical_sha256":"672dbc6aa0d28d00703531675c8b449b74f97f28b409e097d82b620307f0923b","source":{"kind":"arxiv","id":"1209.3554","version":2},"attestation_state":"computed","paper":{"title":"Skyrmions with vector mesons in the hidden local symmetry approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Ghil-Seok Yang, Masayasu Harada, Yong-Liang Ma, Yongseok Oh","submitted_at":"2012-09-17T05:24:30Z","abstract_excerpt":"The roles of light $\\rho$ and $\\omega$ vector mesons in the Skyrmion are investigated in a chiral Lagrangian derived from the hidden local symmetry (HLS) up to $O(p^4)$ including the homogeneous Wess-Zumino (hWZ) terms. We write a general \"master formula\" that allows us to determine the parameters of the HLS Lagrangian from a class of holographic QCD models valid at large $N_c$ and $\\lambda$ ('t Hooft constant) limit by integrating out the infinite towers of vector and axial-vector mesons other than the lowest $\\rho$ and $\\omega$ mesons. Within this approach we find that the physical propertie"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1209.3554","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-09-17T05:24:30Z","cross_cats_sorted":["hep-th","nucl-th"],"title_canon_sha256":"a40b74a6c3d7948a36d83ca2897c3801c897cf2f8d08557b215e372aaf3c1908","abstract_canon_sha256":"4099cd5e9c4c8507ebd29cd367488e5e71da981e65aa31f9bd3d84e59caaff09"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:54:27.506230Z","signature_b64":"4nxpVDilDUnT8xzfJJiBH7aPLPmkbE4gKn0bYDG6VFVi+bgw2xQWVDk9Xj0ZPhlr4EGs+3ae27ILUsjv82sgAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"672dbc6aa0d28d00703531675c8b449b74f97f28b409e097d82b620307f0923b","last_reissued_at":"2026-05-18T01:54:27.505666Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:54:27.505666Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Skyrmions with vector mesons in the hidden local symmetry approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Ghil-Seok Yang, Masayasu Harada, Yong-Liang Ma, Yongseok Oh","submitted_at":"2012-09-17T05:24:30Z","abstract_excerpt":"The roles of light $\\rho$ and $\\omega$ vector mesons in the Skyrmion are investigated in a chiral Lagrangian derived from the hidden local symmetry (HLS) up to $O(p^4)$ including the homogeneous Wess-Zumino (hWZ) terms. We write a general \"master formula\" that allows us to determine the parameters of the HLS Lagrangian from a class of holographic QCD models valid at large $N_c$ and $\\lambda$ ('t Hooft constant) limit by integrating out the infinite towers of vector and axial-vector mesons other than the lowest $\\rho$ and $\\omega$ mesons. Within this approach we find that the physical propertie"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1209.3554","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"1209.3554","created_at":"2026-05-18T01:54:27.505767+00:00"},{"alias_kind":"arxiv_version","alias_value":"1209.3554v2","created_at":"2026-05-18T01:54:27.505767+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1209.3554","created_at":"2026-05-18T01:54:27.505767+00:00"},{"alias_kind":"pith_short_12","alias_value":"M4W3Y2VA2KGQ","created_at":"2026-05-18T12:27:14.488303+00:00"},{"alias_kind":"pith_short_16","alias_value":"M4W3Y2VA2KGQA4BV","created_at":"2026-05-18T12:27:14.488303+00:00"},{"alias_kind":"pith_short_8","alias_value":"M4W3Y2VA","created_at":"2026-05-18T12:27:14.488303+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/M4W3Y2VA2KGQA4BVGFTVZC2ETN","json":"https://pith.science/pith/M4W3Y2VA2KGQA4BVGFTVZC2ETN.json","graph_json":"https://pith.science/api/pith-number/M4W3Y2VA2KGQA4BVGFTVZC2ETN/graph.json","events_json":"https://pith.science/api/pith-number/M4W3Y2VA2KGQA4BVGFTVZC2ETN/events.json","paper":"https://pith.science/paper/M4W3Y2VA"},"agent_actions":{"view_html":"https://pith.science/pith/M4W3Y2VA2KGQA4BVGFTVZC2ETN","download_json":"https://pith.science/pith/M4W3Y2VA2KGQA4BVGFTVZC2ETN.json","view_paper":"https://pith.science/paper/M4W3Y2VA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1209.3554&json=true","fetch_graph":"https://pith.science/api/pith-number/M4W3Y2VA2KGQA4BVGFTVZC2ETN/graph.json","fetch_events":"https://pith.science/api/pith-number/M4W3Y2VA2KGQA4BVGFTVZC2ETN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/M4W3Y2VA2KGQA4BVGFTVZC2ETN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/M4W3Y2VA2KGQA4BVGFTVZC2ETN/action/storage_attestation","attest_author":"https://pith.science/pith/M4W3Y2VA2KGQA4BVGFTVZC2ETN/action/author_attestation","sign_citation":"https://pith.science/pith/M4W3Y2VA2KGQA4BVGFTVZC2ETN/action/citation_signature","submit_replication":"https://pith.science/pith/M4W3Y2VA2KGQA4BVGFTVZC2ETN/action/replication_record"}},"created_at":"2026-05-18T01:54:27.505767+00:00","updated_at":"2026-05-18T01:54:27.505767+00:00"}